In this report we review the present state of the art of the control of propagating quantum
states at the single-electron level and its potential application to quantum information …

Even though bulk metallic systems contain a very large number of strongly interacting
electrons, their properties are well described within Landau's Fermi liquid theory of non …

Ultracold atomic physics offers myriad possibilities to study strongly correlated many-body
systems in lower dimensions. Typically, only ground-state phases are accessible. Using a …

We investigate in detail the behavior of the bipartite fluctuations of particle number N ̂ and
spin S ̂ z in many-body quantum systems, focusing on systems where such U (1) charges …

Recently, there has been growing interest in the creation of artificial magnetic fields for
uncharged particles, such as cold atoms or photons. These efforts are partly motivated by …

The Coulomb phase, with its dipolar correlations and pinch-point–scattering patterns, is
central to discussions of geometrically frustrated systems, from water ice to binary and mixed …

The model of interacting fermion systems in one dimension known as a Tomonaga–
Luttinger liquid (TLL), provides a simple and exactly solvable theoretical framework that …

Coulomb interaction has a striking effect on electronic propagation in one-dimensional
conductors. The interaction of an elementary excitation with neighbouring conductors …

Coulomb interactions have a major role in one-dimensional electronic transport. They
modify the nature of the elementary excitations from Landau quasiparticles in higher …

In contrast to a free-electron system, a Tomonaga–Luttinger (TL) liquid in a one-dimensional
(1D) electron system hosts charge and spin excitations as independent entities,,,. When an …